A gated quantum dot far in the strong-coupling regime of cavity-QED at optical frequencies

The strong-coupling regime of cavity-quantum-electrodynamics (cQED) represents light-matter interaction at the fully quantum level. Adding a single photon shifts the resonance frequencies, a profound nonlinearity. cQED is a test-bed of quantum optics and the basis of photon-photon and atom-atom entangling gates. At microwave frequencies, success in cQED has had a transformative effect. At optical frequencies, the gates are potentially much faster and the photons can propagate over long distances and be easily detected, ideal features for quantum networks. Following pioneering work on single atoms, solid-state implementations are important for developing practicable quantum technology. Here, we embed a semiconductor quantum dot in a microcavity. The microcavity has a \(\mathcal{Q}\)-factor close to \(10^{6}\) and contains a charge-tunable quantum dot with close-to-transform-limited optical linewidth. The exciton-photon coupling rate \(g\) exceeds both the photon decay rate \(\kappa\) and exciton decay rate \(\gamma\) by a large margin (\(g/\gamma=14\), \(g/\kappa=5.3\)); the cooperativity is \(C=2g^{2}/(\gamma \kappa)=150\), the \(\beta\)-factor 99.7%. We observe pronounced vacuum Rabi oscillations in the time-domain, photon blockade at a one-photon resonance, and highly bunched photon statistics at a two-photon resonance. We use the change in photon statistics as a sensitive spectral probe of transitions between the first and second rungs of the Jaynes-Cummings ladder. All experiments can be described quantitatively with the Jaynes-Cummings model despite the complexity of the solid-state environment. We propose this system as a platform to develop optical-cQED for quantum technology, for instance a photon-photon entangling gate.